Solution :
Torque $$\left( \tau \right)$$ acting on a body and angular acceleration $$\left( \alpha \right)$$ produced in it are related as $$\tau = I\alpha $$
Consider a hollow cylinder, around which a rope is wounded as shown in the figure.

Torque acting on the cylinder due to the force $$F$$ is $$\tau = Fr$$
Now, we have $$\tau = I\alpha $$
where, $$I$$ = moment of inertia of the cylinder about the axis through the centre $$ = m{r^2}$$
$$\alpha $$ = angular acceleration
$$\eqalign{
& \Rightarrow \alpha = \frac{\tau }{I} = \frac{{Fr}}{{m{r^2}}} = \frac{F}{{mr}} = \frac{{30}}{{3 \times 40 \times {{10}^{ - 2}}}} \cr
& = \frac{{100}}{4} = 25\,rad/{s^2} \cr} $$